Concept:
The drift velocity of free electrons in a conductor is related to the electric current by the relation
\[
I = neAv_d
\]
where
• \(I\) = current flowing through the conductor,
• \(n\) = number density of free electrons,
• \(e\) = electronic charge,
• \(A\) = area of cross-section of the conductor,
• \(v_d\) = drift velocity of electrons.
For conductors made of the same material, the values of \(n\) and \(e\) are identical.
Step 1: Use the condition of series connection.
The two copper wires are connected in series.
Therefore, the same current flows through both wires.
\[
I_1 = I_2
\]
Using the relation
\[
I = neAv_d
\]
for each wire,
\[
neA_1v_{d1}=neA_2v_{d2}
\]
Cancelling the common factors \(n\) and \(e\),
\[
A_1v_{d1}=A_2v_{d2}
\]
Hence,
\[
\frac{v_{d1}}{v_{d2}}
=
\frac{A_2}{A_1}
\]
Step 2: Express area in terms of radius.
The cross-sectional area of a wire is
\[
A=\pi r^2
\]
Therefore,
\[
\frac{v_{d1}}{v_{d2}}
=
\frac{\pi r_2^2}{\pi r_1^2}
\]
\[
\frac{v_{d1}}{v_{d2}}
=
\frac{r_2^2}{r_1^2}
\]
Step 3: Substitute the given ratio of radii.
Given
\[
r_1:r_2 = 3:2
\]
Therefore,
\[
\frac{v_{d1}}{v_{d2}}
=
\frac{2^2}{3^2}
\]
\[
\frac{v_{d1}}{v_{d2}}
=
\frac{4}{9}
\]
Final Result:
Hence, the ratio of the drift velocities of electrons in the two wires is
\[
\boxed{v_{d1}:v_{d2}=4:9}
\]
Thus, the thinner wire has a larger drift velocity because the same current must pass through a smaller cross-sectional area.